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PII: 0377-0427(89)90022-8
www.damtp.cam.ac.uk/user/ms100/PAPERS/JCAM89.pdf2 Feb 2020: Since. and. ux= [ rx i&r] exp(W,. 24 xx = [ 2irx+, rxx i+,,r - (x)2r] exdih. ... U, = 24, e,_, Sl_le,_2. S,‘e,. Now, for kc n define r&= (AZ)-2e,, and #k= ,S$#Q_, and put 4, = (AZ)-2e,_,. -
Irreversible hydrodynamic trapping by surface rollers
www.damtp.cam.ac.uk/user/lauga/papers/174.pdf6 Jul 2020: magnetic,5 electrostatic,18 or hydrodynamic forces.24 In recentyears, synthetic swimmers actuated by external fields, chemicalfuels or bacteria have been attracting attention and been employedsuccessfully for the transport of cargo ... 23 See ESI†.24 A. -
2. The Integer Quantum Hall E↵ect In this section ...
www.damtp.cam.ac.uk/user/tong/qhe/two.pdf5 Oct 2020: by (1.24). With the Landau levels filled, the current in the x-direction is. ... But we know from (1.20) and (1.24) that these harmonic oscillator states are. -
On the existence of stable and accurate neural networks ...
www.damtp.cam.ac.uk/user/mjc249/pdfs/NN_colbrook10.pdf17 Nov 2020: rL, (24). which is the same estimate as the one dimensional case for boundedd. ... The network weights are providedby the authors of [57] and had been trained on de-identified brainimages from the MGH–USC HCP dataset [24] where the image. -
statphys
www.damtp.cam.ac.uk/user/tong/statphys/five.pdf17 Feb 2020: 5.24). The row of the matrix is specified by the value of si = 1 and the column by si1 = 1. ... siand product over lattice sites. Qiin (5.23) simply tell us. to multiply the matrices defined in (5.24) and the partition function becomes. -
Light-switchable propulsion of active particles with reversible…
www.damtp.cam.ac.uk/user/lauga/papers/175.pdf6 Jul 2020: ARTICLE. Light-switchable propulsion of active particles withreversible interactionsHanumantha Rao Vutukuri 1, Maciej Lisicki 2, Eric Lauga 3 & Jan Vermant 1. Active systems such as microorganisms and self-propelled particles show a plethora of. -
PII: 0022-460X(86)90195-1
www.damtp.cam.ac.uk/user/ms100/PAPERS/JSV86.pdf2 Feb 2020: u,(O) = u(O) = v,(O) = v2(0) = 0. (24). What follows is concerned, not with the general fourth moment at zr but rather with quantities involving intensities at two points -
4.6 Monodromy: the reason for the logarithmic term in ...
www.damtp.cam.ac.uk/user/bg268/Monodromy%20-%20need%20in%20log%20term.pdf11 Mar 2020: 4.6 Monodromy: the reason for the logarithmic term in the solution. Recall that forw′′ p(z)w′ q(z)w = 0, (1). in the vicinity of a RSP at z = 0 (WLOG - other points obtained by translation),there exist two linearly independent solutions of (1), -
3. The Fractional Quantum Hall E↵ect We’ve come to ...
www.damtp.cam.ac.uk/user/tong/qhe/three.pdf5 Oct 2020: i=1. |i|2 (3.24). The corrected plasma partition function is then. Z Yd2zi e. ... precisely by the partition function with energy (3.24) and hence has no dependence. -
3 Supersymmetric Quantum Mechanics We now turn to consider ...
www.damtp.cam.ac.uk/user/dbs26/SUSY/chap3.pdf30 Jan 2020: η̄k1|eτ H(ˆ̄ψ,ψ̂)|ηk〉 = eτ H(η̄k,ηk) 〈η̄k1|ηk〉 = eτ H(η̄k1,ηk) eη̄k1ηk. (3.24).
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